Jump to
S1C2
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -340.374923 |
| Energy at 298.15K | |
| HF Energy | -340.374923 |
| Nuclear repulsion energy | 241.697311 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3120 |
2985 |
32.75 |
|
|
|
| 2 |
A1 |
1944 |
1859 |
480.96 |
|
|
|
| 3 |
A1 |
1592 |
1523 |
1.31 |
|
|
|
| 4 |
A1 |
1384 |
1324 |
0.00 |
|
|
|
| 5 |
A1 |
1146 |
1096 |
192.88 |
|
|
|
| 6 |
A1 |
917 |
877 |
4.95 |
|
|
|
| 7 |
A1 |
787 |
753 |
31.05 |
|
|
|
| 8 |
A1 |
705 |
674 |
1.76 |
|
|
|
| 9 |
A2 |
3153 |
3017 |
0.00 |
|
|
|
| 10 |
A2 |
1275 |
1219 |
0.00 |
|
|
|
| 11 |
A2 |
1148 |
1099 |
0.00 |
|
|
|
| 12 |
A2 |
174i |
166i |
0.00 |
|
|
|
| 13 |
B1 |
3177 |
3039 |
34.38 |
|
|
|
| 14 |
B1 |
1264 |
1209 |
0.14 |
|
|
|
| 15 |
B1 |
876 |
838 |
0.29 |
|
|
|
| 16 |
B1 |
727 |
696 |
26.03 |
|
|
|
| 17 |
B1 |
119 |
114 |
4.41 |
|
|
|
| 18 |
B2 |
3112 |
2978 |
23.54 |
|
|
|
| 19 |
B2 |
1577 |
1508 |
2.39 |
|
|
|
| 20 |
B2 |
1413 |
1352 |
0.01 |
|
|
|
| 21 |
B2 |
1148 |
1098 |
6.61 |
|
|
|
| 22 |
B2 |
961 |
919 |
294.78 |
|
|
|
| 23 |
B2 |
733 |
701 |
0.90 |
|
|
|
| 24 |
B2 |
484 |
463 |
0.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16293.3 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15587.8 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.891 |
| O2 |
0.000 |
0.000 |
2.085 |
| O3 |
0.000 |
1.151 |
0.058 |
| O4 |
0.000 |
-1.151 |
0.058 |
| C5 |
0.000 |
0.782 |
-1.314 |
| C6 |
0.000 |
-0.782 |
-1.314 |
| H7 |
-0.891 |
1.182 |
-1.797 |
| H8 |
0.891 |
1.182 |
-1.797 |
| H9 |
0.891 |
-1.182 |
-1.797 |
| H10 |
-0.891 |
-1.182 |
-1.797 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1934 | 1.4211 | 1.4211 | 2.3400 | 2.3400 | 3.0690 | 3.0690 | 3.0690 | 3.0690 |
O2 | 1.1934 | | 2.3308 | 2.3308 | 3.4877 | 3.4877 | 4.1545 | 4.1545 | 4.1545 | 4.1545 | O3 | 1.4211 | 2.3308 | | 2.3024 | 1.4211 | 2.3705 | 2.0582 | 2.0582 | 3.1112 | 3.1112 | O4 | 1.4211 | 2.3308 | 2.3024 | | 2.3705 | 1.4211 | 3.1112 | 3.1112 | 2.0582 | 2.0582 | C5 | 2.3400 | 3.4877 | 1.4211 | 2.3705 | | 1.5636 | 1.0895 | 1.0895 | 2.2100 | 2.2100 | C6 | 2.3400 | 3.4877 | 2.3705 | 1.4211 | 1.5636 | | 2.2100 | 2.2100 | 1.0895 | 1.0895 | H7 | 3.0690 | 4.1545 | 2.0582 | 3.1112 | 1.0895 | 2.2100 | | 1.7817 | 2.9605 | 2.3644 | H8 | 3.0690 | 4.1545 | 2.0582 | 3.1112 | 1.0895 | 2.2100 | 1.7817 | | 2.3644 | 2.9605 | H9 | 3.0690 | 4.1545 | 3.1112 | 2.0582 | 2.2100 | 1.0895 | 2.9605 | 2.3644 | | 1.7817 | H10 | 3.0690 | 4.1545 | 3.1112 | 2.0582 | 2.2100 | 1.0895 | 2.3644 | 2.9605 | 1.7817 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
110.832 |
|
C1 |
O4 |
C6 |
110.832 |
| O2 |
C1 |
O3 |
125.898 |
|
O2 |
C1 |
O4 |
125.898 |
| O3 |
C1 |
O4 |
108.204 |
|
O3 |
C5 |
C6 |
105.066 |
| O3 |
C5 |
H7 |
109.415 |
|
O3 |
C5 |
H8 |
109.415 |
| O4 |
C6 |
C5 |
105.066 |
|
O4 |
C6 |
H9 |
109.415 |
| O4 |
C6 |
H10 |
109.415 |
|
C5 |
C6 |
H9 |
111.561 |
| C5 |
C6 |
H10 |
111.561 |
|
C6 |
C5 |
H7 |
111.561 |
| C6 |
C5 |
H8 |
111.561 |
|
H7 |
C5 |
H8 |
109.701 |
| H9 |
C6 |
H10 |
109.701 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.879 |
|
|
|
| 2 |
O |
-0.465 |
|
|
|
| 3 |
O |
-0.506 |
|
|
|
| 4 |
O |
-0.506 |
|
|
|
| 5 |
C |
-0.195 |
|
|
|
| 6 |
C |
-0.195 |
|
|
|
| 7 |
H |
0.247 |
|
|
|
| 8 |
H |
0.247 |
|
|
|
| 9 |
H |
0.247 |
|
|
|
| 10 |
H |
0.247 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-5.012 |
5.012 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.893 |
0.000 |
0.000 |
| y |
0.000 |
-37.038 |
0.000 |
| z |
0.000 |
0.000 |
-34.603 |
|
| Traceless |
| | x | y | z |
| x |
3.928 |
0.000 |
0.000 |
| y |
0.000 |
-3.790 |
0.000 |
| z |
0.000 |
0.000 |
-0.138 |
|
| Polar |
| 3z2-r2 | -0.276 |
| x2-y2 | 5.146 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.562 |
0.000 |
0.000 |
| y |
0.000 |
4.526 |
0.000 |
| z |
0.000 |
0.000 |
6.935 |
<r2> (average value of r
2) Å
2
| <r2> |
132.092 |
| (<r2>)1/2 |
11.493 |
Jump to
S1C1
Energy calculated at B1B95/3-21G
| | hartrees |
| Energy at 0K | -340.376025 |
| Energy at 298.15K | -340.382287 |
| HF Energy | -340.376025 |
| Nuclear repulsion energy | 242.402048 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B1B95/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3183 |
3045 |
7.99 |
|
|
|
| 2 |
A |
3099 |
2965 |
16.50 |
|
|
|
| 3 |
A |
1950 |
1865 |
458.92 |
|
|
|
| 4 |
A |
1574 |
1506 |
1.41 |
|
|
|
| 5 |
A |
1399 |
1339 |
5.37 |
|
|
|
| 6 |
A |
1269 |
1214 |
18.99 |
|
|
|
| 7 |
A |
1166 |
1115 |
30.11 |
|
|
|
| 8 |
A |
1120 |
1071 |
130.05 |
|
|
|
| 9 |
A |
938 |
897 |
2.37 |
|
|
|
| 10 |
A |
780 |
746 |
32.58 |
|
|
|
| 11 |
A |
700 |
670 |
2.58 |
|
|
|
| 12 |
A |
140 |
134 |
0.81 |
|
|
|
| 13 |
B |
3194 |
3055 |
19.31 |
|
|
|
| 14 |
B |
3104 |
2970 |
39.02 |
|
|
|
| 15 |
B |
1568 |
1500 |
4.01 |
|
|
|
| 16 |
B |
1412 |
1351 |
0.35 |
|
|
|
| 17 |
B |
1264 |
1209 |
1.25 |
|
|
|
| 18 |
B |
1123 |
1075 |
6.33 |
|
|
|
| 19 |
B |
969 |
927 |
199.57 |
|
|
|
| 20 |
B |
908 |
868 |
75.09 |
|
|
|
| 21 |
B |
739 |
707 |
27.96 |
|
|
|
| 22 |
B |
653 |
625 |
0.68 |
|
|
|
| 23 |
B |
486 |
465 |
0.60 |
|
|
|
| 24 |
B |
134 |
128 |
4.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 16435.0 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 15723.4 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B1B95/3-21G
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.885 |
| O2 |
0.000 |
0.000 |
2.078 |
| O3 |
0.000 |
1.152 |
0.043 |
| O4 |
0.000 |
-1.152 |
0.043 |
| C5 |
0.233 |
0.735 |
-1.301 |
| C6 |
-0.233 |
-0.735 |
-1.301 |
| H7 |
-0.345 |
1.361 |
-1.976 |
| H8 |
1.298 |
0.808 |
-1.533 |
| H9 |
0.345 |
-1.361 |
-1.976 |
| H10 |
-1.298 |
-0.808 |
-1.533 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
O3 |
O4 |
C5 |
C6 |
H7 |
H8 |
H9 |
H10 |
| C1 | | 1.1930 | 1.4270 | 1.4270 | 2.3181 | 2.3181 | 3.1867 | 2.8608 | 3.1867 | 2.8608 |
O2 | 1.1930 | | 2.3383 | 2.3383 | 3.4659 | 3.4659 | 4.2899 | 3.9213 | 4.2899 | 3.9213 | O3 | 1.4270 | 2.3383 | | 2.3048 | 1.4270 | 2.3288 | 2.0588 | 2.0706 | 3.2425 | 2.8307 | O4 | 1.4270 | 2.3383 | 2.3048 | | 2.3288 | 1.4270 | 3.2425 | 2.8307 | 2.0588 | 2.0706 | C5 | 2.3181 | 3.4659 | 1.4270 | 2.3288 | | 1.5416 | 1.0869 | 1.0921 | 2.2047 | 2.1858 | C6 | 2.3181 | 3.4659 | 2.3288 | 1.4270 | 1.5416 | | 2.2047 | 2.1858 | 1.0869 | 1.0921 | H7 | 3.1867 | 4.2899 | 2.0588 | 3.2425 | 1.0869 | 2.2047 | | 1.7888 | 2.8086 | 2.4106 | H8 | 2.8608 | 3.9213 | 2.0706 | 2.8307 | 1.0921 | 2.1858 | 1.7888 | | 2.4106 | 3.0577 | H9 | 3.1867 | 4.2899 | 3.2425 | 2.0588 | 2.2047 | 1.0869 | 2.8086 | 2.4106 | | 1.7888 | H10 | 2.8608 | 3.9213 | 2.8307 | 2.0706 | 2.1858 | 1.0921 | 2.4106 | 3.0577 | 1.7888 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
O3 |
C5 |
108.624 |
|
C1 |
O4 |
C6 |
108.624 |
| O2 |
C1 |
O3 |
126.143 |
|
O2 |
C1 |
O4 |
126.143 |
| O3 |
C1 |
O4 |
107.714 |
|
O3 |
C5 |
C6 |
103.274 |
| O3 |
C5 |
H7 |
109.218 |
|
O3 |
C5 |
H8 |
109.846 |
| O4 |
C6 |
C5 |
103.274 |
|
O4 |
C6 |
H9 |
109.218 |
| O4 |
C6 |
H10 |
109.846 |
|
C5 |
C6 |
H9 |
112.879 |
| C5 |
C6 |
H10 |
111.029 |
|
C6 |
C5 |
H7 |
112.879 |
| C6 |
C5 |
H8 |
111.029 |
|
H7 |
C5 |
H8 |
110.349 |
| H9 |
C6 |
H10 |
110.349 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.876 |
|
|
|
| 2 |
O |
-0.464 |
|
|
|
| 3 |
O |
-0.502 |
|
|
|
| 4 |
O |
-0.502 |
|
|
|
| 5 |
C |
-0.199 |
|
|
|
| 6 |
C |
-0.199 |
|
|
|
| 7 |
H |
0.250 |
|
|
|
| 8 |
H |
0.245 |
|
|
|
| 9 |
H |
0.250 |
|
|
|
| 10 |
H |
0.245 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-4.924 |
4.924 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.937 |
0.292 |
0.000 |
| y |
0.292 |
-37.095 |
0.000 |
| z |
0.000 |
0.000 |
-34.383 |
|
| Traceless |
| | x | y | z |
| x |
3.803 |
0.292 |
0.000 |
| y |
0.292 |
-3.935 |
0.000 |
| z |
0.000 |
0.000 |
0.132 |
|
| Polar |
| 3z2-r2 | 0.265 |
| x2-y2 | 5.159 |
| xy | 0.292 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.663 |
0.132 |
0.000 |
| y |
0.132 |
4.446 |
0.000 |
| z |
0.000 |
0.000 |
6.899 |
<r2> (average value of r
2) Å
2
| <r2> |
130.622 |
| (<r2>)1/2 |
11.429 |